3,339 research outputs found

    Schiff Theorem and the Electric Dipole Moments of Hydrogen-Like Atoms

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    The Schiff theorem is revisited in this work and the residual PP- and TT-odd electron--nucleus interaction, after the shielding takes effect, is completely specified. An application is made to the electric dipole moments of hydrogen-like atoms, whose qualitative features and systematics have important implication for realistic paramagnetic atoms.Comment: 3 pages. Contribution to PANIC05, Particles and Nuclei International Conference, Santa Fe, New Mexico, Oct. 24-28, 200

    Recovery Is Up to You, a peer-run course

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    Atomic Electric Dipole Moments: The Schiff Theorem and Its Corrections

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    Searches for the permanent electric dipole moments (EDMs) of diamagnetic atoms provide powerful probes of CP-violating hadronic and semileptonic interactions. The theoretical interpretation of such experiments, however, requires careful implementation of a well-known theorem by Schiff that implies a vanishing net EDM for an atom built entirely from point-like, nonrelativistic constituents that interact only electrostatically. Any experimental observation of a nonzero atomic EDM would result from corrections to the point-like, nonrelativistic, electrostatic assumption. We reformulate Schiff's theorem at the operator level and delineate the electronic and nuclear operators whose atomic matrix elements generate corrections to "Schiff screening". We obtain a form for the operator responsible for the leading correction associated with finite nuclear size -- the so-called "Schiff moment" operator -- and observe that it differs from the corresponding operator used in previous Schiff moment computations. We show that the more general Schiff moment operator reduces to the previously employed operator only under certain approximations that are not generally justified. We also identify other corrections to Schiff screening that may not be included properly in previous theoretical treatments. We discuss practical considerations for obtaining a complete computation of corrections to Schiff screening in atomic EDM calculations.Comment: 31 pages, 2 figures, typeset by REVTe

    On-line Excited-State Laser Spectroscopy of Trapped Short-Lived Ra+^+ Ions

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    As an important step towards an atomic parity violation experiment in one single trapped Ra+^+ ion, laser spectroscopy experiments were performed with on-line produced short-lived 212,213,214^{212,213,214}Ra+^+ ions. The isotope shift of the 6\,^2D3/2_{3/2}\,-\,7\,^2P1/2_{1/2} and 6\,^2D3/2_{3/2}\,-\,7\,^2P3/2_{3/2} transitions and the hyperfine structure constant of the 7\,^2S1/2_{1/2} and 6\,^2D3/2_{3/2} states in 213^{213}Ra+^+ were measured. These values provide a benchmark for the required atomic theory. A lower limit of 232(4)232(4) ms for the lifetime of the metastable 6\,^2D5/2_{5/2} state was measured by optical shelving.Comment: 4.2 pages, 6 figures, 2 tables

    Stationary solutions of the one-dimensional nonlinear Schroedinger equation: II. Case of attractive nonlinearity

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    All stationary solutions to the one-dimensional nonlinear Schroedinger equation under box or periodic boundary conditions are presented in analytic form for the case of attractive nonlinearity. A companion paper has treated the repulsive case. Our solutions take the form of bounded, quantized, stationary trains of bright solitons. Among them are two uniquely nonlinear classes of nodeless solutions, whose properties and physical meaning are discussed in detail. The full set of symmetry-breaking stationary states are described by the CnC_{n} character tables from the theory of point groups. We make experimental predictions for the Bose-Einstein condensate and show that, though these are the analog of some of the simplest problems in linear quantum mechanics, nonlinearity introduces new and surprising phenomena.Comment: 11 pages, 9 figures -- revised versio

    Periodically-dressed Bose-Einstein condensates: a superfluid with an anisotropic and variable critical velocity

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    Two intersecting laser beams can produce a spatially-periodic coupling between two components of an atomic gas and thereby modify the dispersion relation of the gas according to a dressed-state formalism. Properties of a Bose-Einstein condensate of such a gas are strongly affected by this modification. A Bogoliubov transformation is presented which accounts for interparticle interactions to obtain the quasiparticle excitation spectrum in such a condensate. The Landau critical velocity is found to be anisotropic and can be widely tuned by varying properties of the dressing laser beams.Comment: 5 pages, 4 figure

    A microscopic quantum dynamics approach to the dilute condensed Bose gas

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    We derive quantum evolution equations for the dynamics of dilute condensed Bose gases. The approach contains, at different orders of approximation, for cases close to equilibrium, the Gross Pitaevskii equation and the first order Hartree Fock Bogoliubov theory. The proposed approach is also suited for the description of the dynamics of condensed gases which are far away from equilibrium. As an example the scattering of two Bose condensates is discussed.Comment: 8 pages, submitted to Phys. Rev.

    First Test of Lorentz Invariance in the Weak Decay of Polarized Nuclei

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    A new test of Lorentz invariance in the weak interactions has been made by searching for variations in the decay rate of spin-polarized 20Na nuclei. This test is unique to Gamow-Teller transitions, as was shown in the framework of a recently developed theory that assumes a Lorentz symmetry breaking background field of tensor nature. The nuclear spins were polarized in the up and down direction, putting a limit on the amplitude of sidereal variations of the form |(\Gamma_{up} - \Gamma_{down})| / (\Gamma_{up} + \Gamma_{down}) < 3 * 10^{-3}. This measurement shows a possible route toward a more detailed testing of Lorentz symmetry in weak interactions.Comment: 11 pages, 6 figure
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